Almost Everywhere Convergence of Inverse Dunkl Transform on the Real Line

dc.creatorKamel, Jamel El
dc.creatorYacoub, Chokri
dc.date2007-06-25
dc.date.accessioned2026-07-07T08:12:13Z
dc.date.available2026-07-07T08:12:13Z
dc.descriptionIn this paper, we will first show that the maximal operator $S_*^α$ of spherical partial sums $S_R^α$, associated to Dunkl transform on $\mathbb{R}$ is bounded on $L^p(\mathbb{R}, |x|^{2α+1} dx)$ functions when $\frac{4(α+1)}{2α+3}<p<\frac{4(α+1)}{2α+1}$, and it implies that, for every $L^p(\mathbb{R}, |x|^{2α+1} dx)$ function $f(x)$, $S_R^αf(x)$ converges to $f(x)$ almost everywhere as $R\to \infty$. On the other hand we obtain a sharp version by showing that $S_*^α$ is bounded from the Lorentz space $L^{p_i,1}(\mathbb{R}, |x|^{2α+1})$ into $L^{p_i,\infty}(\mathbb{R}, |x|^{2α+1}),\quad i=0,1$ where $p_0=\frac{4(α+1)}{2α+3}$ and $p_1=\frac{4(α+1)}{2α+1}$.
dc.description9 pages
dc.identifierhttps://arxiv.org/abs/0706.3619
dc.identifierhttp://arxiv.org/abs/0706.3619
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/132378
dc.subjectClassical Analysis and ODEs
dc.titleAlmost Everywhere Convergence of Inverse Dunkl Transform on the Real Line
dc.typetext

Files

Collections